Strain measurement

• US 4,173,412 A
• Filed: 06/29/1977
• Issued: 11/06/1979
• Est. Priority Date: 07/01/1976
• Status: Expired due to Term

• Current Assignee: International Standard Electric Corporation (ITT, Inc.)
• Original Assignee: International Standard Electric Corporation (ITT, Inc.)
• Inventors: Wright, Stephen, Ramsay, Melvin M.
• Primary Examiner(s): Corbin, John K.
• Assistant Examiner(s): Punter, Wm. H.
• Application Number:
  US05/811,008
• Time in Patent Office: 860 Days
• Field of Search: 356/32-35, 356/114-117, 356/239, 356/365, 356/73.1, 73/88 A
• US Class Current: 356/33
• CPC Class Codes: G01B 11/18 using photoelastic elements
• CPC Class Codes: G01L 1/243 using means for applying force perpendicular to the fibre axis
• CPC Class Codes: G01L 11/025 using a pressure-sensitive optical fibre

Abstract

A strain sensor providing an optical read-out that is suitable for use in electrically noisy environment or one subject to mechanical vibration consists of one or a set of single mode optical fibres wound round an expanding strain member. The principle of operation relies upon the fact that transverse straining of a single mode fibre destroys mode degeneracy thereby producing birefringence effects that can be rendered obversable using polarized light and a polarization analyzer.

Claims

1. A method of measuring the magnitude of strain in at least one optical fiber of circular symmetry comprising the steps of:

straining the fiber over a portion of its length in a direction perpendicular to the fiber axis;

propagating polarized light through the fiber while under strain;

monitoring the polarized light propagating through the fiber to determine the strain-induced difference in phase velocity of two orthogonal fundamental modes of the propagated light;

wherein the strain is applied to one single fiber and wherein the strain induced phase velocity difference of the two orthogonal fundamental modes is measured by polarized light having components in and perpendicular to the strain direction into one end of the fiber and exiting the light from another end of the fiber; and

splitting the light emerging from the fiber into two components each of said components passing to an associated photodetector through an associated linear polarization analyzer having a polarization axis aligned at 45°

to the strain direction wherein only one of said analyzers is prefaced with a quarter-waveplate with its optic axis aligned at 45°

to the polarization axis of the analyzer.

2. The method of claim 1 wherein the polarised light propagates with a normalised frequency of less than 2.405.

3. The method of claim 1 including the step of using changes occuring at the outputs of the detectors to control the value of the count in a counter the value of the count being changed by one unit each time the output of a particular one of the counters passes through a median threshold value, increasing or decreasing the count according to whether the strain is increasing or decreasing as determined having regard to whether the magnitude of the output of the one detector is increasing or decreasing at the instant output of the other detector at the instant of the passage of the output of the one detector through the threshold decreasing as determined having regard firstly to whether the output is increasing or decreasing in its passage through the threshold value and secondly to the magnitude of the output of the other detector at the instant of said passage through the threshold value.

4. A method of measuring the magnitude of strain in at least one optical fiber of circular symmetry comprising the steps of straining the fiber over a portion of its length in a direction perpendicular to the fiber axis;

propagating polarized light through the fiber while under strain;

monitoring the polarized light propagating through the fiber to determine the strain-induced difference in phase velocity of two orthogonal fundamental modes of the propagated light;

wherein the strain is applied to a set of fibers over portions of their length that are in harmonic relationship such that each strained length is twice the strained length of its predecessor in the set, and wherein the strain induced phase velocity difference of the two orthogonal fundamental modes is measured by directing polarized light having components in and perpendicular to the strain direction through each fiber, by directing the light emerging therefrom through a linear polarization analyzer, whose polarization axis is aligned at 45°

to the strain direction, to an associated photodetector, and by deriving a coded binary representation of the magnitude of the applied strain by determining whether the individual detector outputs are above or beneath a median threshold value.

5. A method of measuring the magnitude of strain in at least one optical fiber of circular symmetry comprising the steps of straining the fiber over a portion of its length in a direction perpendicular to the fiber axis;

propagating polarized light through the fiber while under strain; and

monitoring the polarized light propagating through the fiber to determine the strain-induced difference in phase velocity of two orthogonal fundamental modes of the propagated light;

wherein the strain is applied to a set of fibers over portions of their length that are in harmonic relationship such that each strained length is four times the strained length of its predecessor in the set, and wherein the strain induced phase velocity difference of the two orthogonal fundamental modes is measured by directing polarized light having components in and perpendicular to the strain direction through each fiber, by splitting the light emerging therefrom into two components each of which passes to an associated photodetector through an associated linear polarization analyzer whose polarization axis is aligned at 45°

to the strain direction wherein only one of the two analyzers associated with each fiber is prefaced with a quarter-waveplate with its optic axis aligned at 45°

to the polarization axis of the analyzer, and by deriving a coded binary digital representation of the magnitude of the applied strain by determining whether the individual detector outputs are above or beneath a median threshold value.

6. A strain sensor as claimed in claim 5 wherein the strain member is a hollow vessel.

7. A strain sensor including a light source, an optical fibre of circular symmetry wrapped around a strain member such that expansion of the strain member strains the wrapped around portion of the fibre in a direction perpendicular to its axis, a beam splitter, a quarter-waveplate, and a pair of photodetectors whose outputs are connected to a pair of threshold switching devices, wherein the light source is adapted to launch polarised light into one end of the fibre to excite two orthogonal fundamental modes propagating with a normalised frequency of less than 2.405, one mode having its polarisation direction aligned with the strain direction, wherein the other end of the fibre is positioned with respect to the beam splitter to divide the light that has propagated therethrough into a pair of beams which are directed to the photodetectors each beam reaching its photodetector via a linear polarisation analyser whose polarisation direction is inclined at 45°

to the fibre strain direction and wherein a single one of the beams reaches its analyser via a quarter-waveplate oriented with its optic axis at 45°

to the polarisation direction of the analyser.

8. A strain sensor as claimed in claim 7 wherein the optical fibre is made of silica.

9. A strain sensor including at least one light source, a set of optical fibres of circular symmetry and identical construction wrapped around a strain member such that expansion of the strain member strains the wrapped around portion of each fibre of the set in a direction perpendicular to its axis, one or more linear polarisation analysers, and a set of photodetectors each of whose outputs is connected to the input of an associated one of a set of threshold switching devices, wherein the individual lengths of the wrapped around portions of the set of fibres are harmonically related such that the wrapped around length of each fibre is twice the wrapped around length of its predecessor in the set of fibres, wherein the light source is adapted to launch polarised light into one end of each member of the set fibres to excite two orthogonal fundamental modes propagating with a normalised frequency of less than 2.405, one mode having its polarisation direction aligned with the strain direction, and wherein the other end of each member of the set of fibres is positioned to direct light that has propagated therethrough to an associated one of the set of photodetectors via the, or one of the, linear polarisation analysers oriented with its polarisation direction at 45°

to the fibre strain direction.

10. A strain sensor including at least one light source, a set of optical fibres of circular symmetry and identical construction wrapped around a strain member such that expansion of the strain member strains the wrapped around portion of each fibre of the set in a direction perpendicular to its axis, at least one beam splitter, one or more quarter-waveplates, at least one linear polarisation analyser, and a set of photodetectors having a plurality of outputs each connected to the input of an associated one of a set of threshold switching devices, wherein the individual lengths of the wraped around portions of the set of fibres are harmonically related such that the wrapped around length of each fibre is four times the length of its predecessor in the set of fibres, wherein the light source or sources are adapted to launch polarised light into one end of each member of the set of fibres to excite two orthogonal fundamental modes propagating with a normalised frequency of less than 2.405, one mode having its polarisation direction aligned with the strain direction, wherein the other end of each member of the set of fibres is positioned with respect to the beam splitter to divide light that has propagated therethrough into a pair of beams directed to an associated pair of members of the set of photodetectors each beam reaching its photodetector via the linear polarisation analyser said analyser being oriented with its polarisation direction at 45°

to the fibre strain direction and wherein the quarter-waveplate is disposed such that a single member of each pair of beams reaches its associated analyser via a quarter-waveplate oriented with the optic axis aligned at 45°

to the polarisation direction of the analyser.